JP2011206013A - Spinning reel - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a spinning reel in which the flying distance or operability (backlash prevention) can be improved by braking an energizing force from an initial period of casting to a later period of casting to be adjusted to deal with various casting conditions (such as the throw-in method, the lure to be used and the wind direction), and a degree of freedom in design of the braking force is improved by eliminating the problem in space.SOLUTION: A spinning reel 10 includes a magnetic braking device 40 in which a non-magnetic conductor 50 whirl-stopped on a spool shaft 14 is movable away from a spool 18 along with an axial direction of the spool shaft 14 with a centrifugal force with rotations of the spool and which magnetically brakes the rotations of the spool via the conductor while the conductor is located within a magnetic field between confronted magnets 74, 76. The conductor 50 then includes two regions 52, 54 having respectively different conductivities, and the two regions can be disposed within the magnetic field between the magnets 74, 76.

Description

  The present invention relates to a fishing reel provided with a magnetic braking device that applies a braking force to a spool that is rotatably supported by a reel body to prevent backlash during a fishing line releasing operation.

As a known example, there is a known technique for changing a braking force between an initial stage and an end stage of casting in a magnetic braking apparatus that prevents backlash during a fishing line releasing operation of a fishing reel.
For example, the fishing reel disclosed in Patent Document 1 eliminates the suppression of the spool rotation speed at the initial and final stages of casting, and increases the flying distance of the device and prevents the occurrence of backlash. The radial movement of the roller is converted into the axial direction, and the electric conductor provided in the centrifugal collar can be moved back and forth in the magnetic field in the reel body against the urging force. While the spool rotates at a low speed, the conductor is disposed outside the magnetic field by the action of the urging force, so that no braking force is generated on the spool. For this reason, unnecessary suppression of spool rotation is eliminated at the initial rising of casting, the rising is smooth, and the flight distance can be improved as compared with the conventional magnetic braking device.
Further, in the fishing reel of Patent Document 2, the spool can be smoothly rotated at the beginning of casting to improve the flying distance of the device, and the flying distance is unnecessarily reduced at the end of casting. As a method that can effectively prevent backlash by applying an appropriate braking force to the spool without causing the spool to rotate, the radial gap between the conductor and the magnet along with the axial movement of the conductor due to the rotation of the spool Is changing.

Japanese Patent No. 3515875 JP 2008-245552 A

In the fishing reel of Patent Document 1, the urging force acts in the direction of moving the conductor away from the inside of the magnetic field at the end of casting, so that the conductor is suddenly returned to the outside of the magnetic field when the rotation speed of the spool is reduced. The brake force applied to the spool via this will not work.
Further, in order to change the gap amount between the conductor and the magnet in the fishing reel of Patent Document 2, a sufficiently large space is required. In particular, if the base side of the conductor is thin, the rigidity of the conductor is insufficient, and the conductor may be deformed by the centrifugal force due to the rotation of the spool and contact the magnet. In that case, additional space is required between the conductor and the magnet. Therefore, there is a limit to the degree of design freedom.

  The present invention has been made in view of the above problems, and its object is to adjust the braking force from the initial stage to the late stage in order to cope with various casting conditions (such as charging method, used lure, and wind direction). This makes it possible to improve the flight distance and operability (prevention of backlash), and there is no problem in the space between the conductor and the magnet. It is to provide.

In order to solve the above-described problems, in the fishing reel according to the present invention, the non-magnetic conductor that is prevented from rotating on the spool shaft is moved along the axial direction of the spool shaft by the centrifugal force caused by the rotation of the spool. And a magnetic braking device that magnetically brakes rotation of the spool via the conductor when the conductor is in a magnetic field between opposing magnets, the conductors being respectively It has at least two regions having different conductivity, and the at least two regions can be disposed in a magnetic field between the magnets.
In the conductor, it is preferable that the conductivity of the region close to the spool is higher than the conductivity of the region separated from the spool.
In the conductor, it is preferable that the specific gravity of the region adjacent to the spool is higher than the specific gravity of the region separated from the spool.
The conductor is cylindrical and has a first conductive member arranged from a side close to the spool to a side away from the spool, and an outer side of the first conductive member on the side separated from the spool. A second conductive member disposed on the first conductive member, and the conductor is adjacent to the spool of the second conductive member from a side of the first conductive member adjacent to the spool. Forming a first region defined in a range of the end portion on the side to be connected and a second region defined in a range in which the first and second conductive members are overlapped with each other. It is preferable that the conductivity be constant.
The opposing magnets have a width in the direction of movement of the electric conductor, and when the electric conductor moves in a direction away from the spool, the side of the electric conductor that is separated from the spool faces the opposite side. It is preferable that the magnet can penetrate through the magnetic field and move deeper than the width of the magnet.
Further, it is preferable that the magnetic braking device further includes an axial movement holding mechanism that holds the opposing magnets so as to be movable in the axial direction of the spool shaft.

According to the present invention, the conductor has at least two regions each having different conductivity, and these regions can be arranged in the magnetic field between the magnets, thereby giving a difference in the magnitude of the braking force, Different braking performance can be exhibited in each region. For this reason, the braking force can be adjusted from the initial stage to the late stage by setting the braking performance for each conductor area according to various casting conditions (such as throwing method, used lure, and wind direction). And operability (prevention of backlash) can be improved, and there is no problem in terms of space, and the degree of freedom in designing the braking force can be increased.
In addition, by making the conductivity of the region on the side close to the spool higher than the conductivity of the region on the side separated from the spool, the conductor is moved between the magnets as the rotational speed of the spool increases from the initial state. When braking, the braking force can be gradually increased.
Further, by making the specific gravity of the region close to the spool higher than the specific gravity of the region separated from the spool, it is possible to reduce the weight of the conductor while keeping the weight separated from the spool low. , The moment of inertia can be reduced, and good braking performance can be obtained.
By forming the first region with the first conductive member on the side close to the spool and forming the second region with the first and second conductive members on the side separated from the spool, The braking performance can be set easily.
By making the conductor move in the axial direction of the spool shaft beyond the range of the magnet, it is possible to easily arrange regions having various conductivity between the magnets.
Since the initial position of the magnet with respect to the conductor can be moved toward and away by the axial movement holding mechanism, regions having various conductivity can be easily arranged between the magnets according to the casting conditions.

The schematic fragmentary sectional view which shows the fishing reel which concerns on 1st to 3rd embodiment. 1 is a schematic cross-sectional view showing a fishing brake magnetic braking device according to a first embodiment. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 schematically shows a fishing brake magnetic braking device according to a first embodiment, wherein (A) shows a state in which a spool shaft and a spool are stopped and a conductor is outside between magnets, and (B) shows a spool. The moving body moves along the axial direction of the spool shaft by the centrifugal force due to the rotation of the shaft and the spool, and shows a state where the second region of the conductor is between the magnets. The figure which shows the state in which all the 2nd area | regions of a conductor and a part of 1st area | region exist between magnets because force further increases and a moving body moves along the axial direction of a spool axis | shaft. The magnetic braking device of the fishing reel concerning a 2nd embodiment is shown roughly, (A) shows the state where a spool axis and a spool are in a stop state, and only the tip side of the 2nd field of a conductor is between magnets. , (B) shows a state in which the movable body moves along the axial direction of the spool shaft by the centrifugal force due to the rotation of the spool shaft and the spool, and the entire second region of the conductor is between the magnets, and (C) is the spool. The figure which shows the state in which the centrifugal force by rotation of an axis | shaft and a spool becomes larger, a moving body moves along the axial direction of a spool axis | shaft, and the 2nd area | region of a conductor and a part of 1st area | region exist between magnets. FIG. 5 schematically shows a fishing brake magnetic braking device according to a third embodiment, where (A) shows a state where the spool shaft and the spool are stopped and the entire third region of the conductor is between the magnets; ) Shows a state in which the moving body moves along the axial direction of the spool shaft by the centrifugal force generated by the rotation of the spool shaft and the spool, and the entire third region and the second region of the conductor are between the magnets. The centrifugal force due to the rotation of the spool shaft and the spool is further increased, and the moving body moves along the axial direction of the spool shaft so that the entire second region of the conductor and a part of the first region are between the magnets. FIG. The schematic fragmentary sectional view which shows the fishing reel which concerns on 4th Embodiment. The schematic cross-sectional view which shows the state which separated the magnet of the magnetic braking device of the fishing reel which concerns on 4th Embodiment with respect to the spool. The schematic cross-sectional view which shows the state which made the magnet of the magnetic braking device of the fishing reel which concerns on 4th Embodiment adjoin with respect to a spool. FIG. 9 is a diagram schematically showing a cam action when a magnet is separated or close to a spool in the configuration shown in FIGS. 7 and 8. Sectional drawing along the XX line of FIG. 7 and FIG. FIG. 7 schematically shows the state of FIG. 7 in which the magnet of the magnetic brake device for a fishing reel according to the fourth embodiment is separated from the spool, where (A) shows the state in which the spool shaft and the spool are stopped and the conductor is a magnet. (B) shows the state where the movable body moves along the axial direction of the spool shaft by the centrifugal force caused by the rotation of the spool shaft and the spool, and only the tip side of the second region of the conductor is between the magnets. (C) shows that the centrifugal force due to the rotation of the spool shaft and the spool is further increased, and the moving body moves along the axial direction of the spool shaft so that only the second region of the conductor is between the magnets. FIG. FIG. 8 schematically shows the state of FIG. 8 in which the magnet of the magnetic brake device for a fishing reel according to the fourth embodiment is brought close to the spool, and FIG. FIG. 2B shows a state where only the tip side of one region is outside the magnet, and FIG. 5B shows a state in which the moving body moves along the axial direction of the spool shaft by the centrifugal force caused by the rotation of the spool shaft and the spool, (C) shows a state in which the entire region is between the magnets, and (C) shows that the centrifugal force due to the rotation of the spool shaft and the spool is further increased, and the moving body moves along the axial direction of the spool shaft. The figure which shows the state in which each 1st area | region exists between magnets. The magnetic brake device of the fishing reel which concerns on 5th Embodiment is shown, a spool axis | shaft and a spool are a stop state, the state which has a conductor on the outer side between magnets, a conductor is the 1st conductive member and 2nd FIG. 5 is a schematic cross-sectional view showing a state in which the first region and the second region are formed by the first and second conductive members formed with the conductive member. The magnetic braking device of the fishing reel which concerns on 6th Embodiment is shown, a spool axis | shaft and a spool are in a stop state, the state which has a conductor on the outer side between magnets, a conductor is the 1st conductive member and 2nd FIG. 6 is a schematic cross-sectional view showing a state where the first region, the second region, and the third region are formed by the first and second conductive members.

Hereinafter, embodiments for carrying out the present invention will be described with reference to the drawings.
A first embodiment will be described with reference to FIGS. 1 to 3.
As shown in FIG. 1, a double-bearing reel 10 as a fishing reel according to the present embodiment includes left and right side plates 10a and 10b and left and right frames 12a and 12b covered with both side plates 10a and 10b. It has a reel body. A spool shaft 14 is rotatably supported between the left and right frames 12a and 12b via a pair of bearings 16a and 16b, and a spool 18 around which a fishing line is wound is disposed on the outer periphery of the spool shaft 14. It is fixed integrally.

A pinion gear 20 that is movable along the axial direction of the spool shaft 14 is attached to the end of the spool shaft 14 that protrudes from the right frame 12b. A drive gear 22 meshes with the pinion gear 20, and a handle 26 is attached to one end of a handle shaft 24 that is attached to the drive gear 22 and rotatably supported by the right side plate 10 b of the reel body 12. Therefore, when the handle 26 is rotated, the drive gear 22 is rotated via the handle shaft 24 and the pinion gear 20 is rotated.
The pinion gear 20 is engaged with the spool shaft 14 and rotated together with the spool shaft 14 by a known switching means (not shown) interlocked with a clutch lever 28 disposed between the outer plates 10a and 10b (power transmission). State) and a disengaged position (power cutoff state) where the engagement state with the spool shaft 14 is released. For example, when the clutch lever 28 is pushed down from the position where it is engaged with the spool shaft 14 shown in FIG. 1, the clutch plate 28 a moves to the right in FIG. 1, and the pinion gear 20 can be separated from the spool shaft 14. When the handle 26 is rotated in the separated state, the pinion gear 20 is fitted to the spool shaft 14 via a known return mechanism (not shown) to return to the original state (winding state) and integrated with the spool shaft 14. The formed spool 18 and pinion gear 20 rotate integrally.

  A known level winding device 30 is disposed between the left and right frames 12a and 12b on the side of the spool 18 in the direction of feeding the fishing line. The level wind device 30 is configured so that the fishing line guide 32 through which the fishing line is inserted moves left and right by rotating the handle 26, and the fishing line is evenly distributed to the spool 18 as the fishing line is wound up. Wind.

In the present embodiment, a magnetic braking device 40 that prevents over-rotation of the spool 18 during the fishing line releasing operation is disposed on the left side plate 10a side.
The magnetic braking device 40 includes a cylindrical moving body 42 that is disposed on the outer peripheral surface of the spool shaft 14, is movable in the axial direction, and is fitted on the outer peripheral shaft of the spool shaft 14. Yes. On the outer peripheral surface of the moving body 42, a notch-shaped support member 42 a formed by extending in the radial direction at a predetermined interval is formed, and each support member 42 a has an axial direction of the spool shaft 14. A centrifugal collar (radial direction moving member) 44 is supported so as to be movable in the orthogonal radial direction. When the spool shaft 14 (and the moving body 42) rotates together with the spool 18, these centrifugal collars 44 move radially outward with respect to the support member 42a by centrifugal force.

  A cylindrical conductor 50 made of a nonmagnetic conductive material is fixedly supported on one side (left frame 12a side) of the support member 42a of the moving body 42, that is, on the side opposite to the handle 26. The conductor 50 is movable along the axial direction of the spool shaft 14 as the movable body 42 moves in the axial direction of the spool shaft 14.

  A taper surface (guide surface) 18a is formed on the back side of the fishing line winding surface of the spool 18 as an axial direction conversion control unit that gradually increases in diameter toward the left frame 12a. When the centrifugal collar 44 moves radially outward, the tapered surface 18a is brought into surface contact (engagement) with an inclined surface 44a formed on the outer surface of the centrifugal collar 44 to guide the movement of the centrifugal collar 44. That is, the centrifugal collar 44 supported by the support member 42a of the moving body 42 is moved in the radial direction by the engaging action with the inclined surface 44a by the centrifugal force accompanying the rotation of the spool shaft 14 (spool 18), and is tapered. The movable body 42 guided along the surface 18a and supporting the annular conductor 50 is moved toward the left frame 12a along the axial direction of the spool shaft 14 (the radial movement of the centrifugal collar 44). Is converted into an axial movement of the moving body 42).

  Between the retainer 46 fixed to one end of the spool shaft 14 and the moving body 42, a spring member 48 that constantly urges the moving body 42 toward the spool 18 is inserted. For this reason, the conductor 50 is always urged in the direction away from the magnetic field in the high magnetic flux density range α between the magnets 74 and 76 described later (on the spool 18 side). In this embodiment, as shown in FIG. 3C, the moving body 42, the retainer 46, and the spring member 48 are formed of a conductor 50 for the support member 42a of the moving body 42 when the spring member 48 is contracted most. This prevents the distal end of the magnet 74, 76 from coming out to the left side (left side plate 10a side) from the left side ends of the magnets 74 and 76. That is, the width L of the magnets 74 and 76 (the length of the magnets 74 and 76 along the axial direction of the spool shaft 14) L is substantially equal to the movable distance of the moving body 42.

The conductor 50 is formed on the distal side of the first region 52 from the support member 42a and the cylindrical first region 52 extending from the support member 42a of the moving body 42 toward the left side plate 10a. A cylindrical second region 54 is defined. In this embodiment, the first and second regions 52 and 54 have the same thickness, and the boundary portion between the first region 52 and the second region 54 is, for example, fitted, bonded, or a combination thereof. It is fixed by various means. The conductor 50 is made of a non-magnetic conductive material. Among the conductors 50, the first region 52 near the support member 42 a of the moving body 42 and the second region 52 away from the support member 42 a of the moving body 42. The conductivity of the region 54 is different. The first region 52 is made of a material having a higher conductivity than that of the second region 54. For the first region 52, for example, a Cu alloy (JIS C1220T, conductivity 86 (IACS), specific gravity 8.94, Young's modulus 11800 (kgf / mm ² )) shown in Table 1 below is used. For example, an Al alloy (JIS A2011-T3, conductivity 39 (IACS), specific gravity 2.82, Young's modulus 7200 (kgf / mm ² )) is used for the second region 54.
Of course, other materials shown in Table 1 may be used as long as the electrical conductivity relationship between the first region 52 and the second region 54 can be maintained. That is, for example, a Cu alloy shown in Table 1 is used for the first region 52 and an Mg alloy is used for the second region 54, or an Al alloy shown in Table 1 is used for the first region 52 and Mg is used for the second region 54. It is also possible to use an alloy. In addition, materials other than those shown in Table 1 may be used as appropriate.

  The magnetic braking device 40 includes a support plate 60 that rotatably supports the end of the spool shaft 14 via a bearing 16a on the inner surface side of the left plate 10a facing the conductor 50. The support plate 60 is a left plate. For example, a plurality of screws are firmly fixed to 10a. The support plate 60 has a support base 68 having a stepped structure in which a small diameter portion 64 and a large diameter portion 66 are formed in order from the tip side, that is, the spool 18 side, coaxially with the central opening 62 that accommodates the bearing 16a. An annular groove 70 for accommodating a magnet holder 72 described later is formed in the peripheral portion of the support base 68.

An inner ring magnet 74 is fixed to the small-diameter portion 64 of the support plate 60. The inner ring magnet 74 is formed by alternately magnetizing a plurality of pairs of N and S poles that orient the magnetic field in the radial direction. is there. A magnet holder 72 disposed in the annular groove 70 is slidably mounted in the circumferential direction on the large-diameter portion 66, and is attached to the inner peripheral side of the magnet holder 72 in the direction opposite to the inner ring magnet 74. A magnetized outer ring magnet 76 is fixed. That is, a high magnetic flux density range α is formed in the gap between the magnets 74 and 76. The conductor 50 described above is disposed so as to be able to advance and retreat with respect to an annular gap formed between the inner ring magnet 74 and the outer ring magnet 76, thereby forming the magnetic braking device 40.
Accordingly, when the conductor 50 is rotated in the gap between the inner ring magnet 74 and the outer ring magnet 76 as the spool 18 that discharges the fishing line rotates, the eddy current generated in the conductor 50 causes the spool 18 to rotate. A force in the direction opposite to the rotation direction acts as a braking force to magnetically brake the spool 18 that prevents the conductor 50 from rotating.
The widths L of the magnets 74 and 76 may be different from each other. In this case, the range in which the magnets 74 and 76 face each other in the width direction (the axial direction of the spool shaft 14) is the high magnetic flux density range α. Become.

In order to adjust the braking force acting on the spool 18, teeth 78 (see FIG. 2) are formed on at least a part of the outer periphery of the magnet holder 72, and the teeth 78 are disposed through the openings 60 a of the support plate 60. In this embodiment, a braking force adjusting knob 82 for rotating a small gear 84 meshingly engaged via the intermediate gear 80 is disposed on the left outer plate 10a.
When the braking force adjusting knob 82 is rotated, the magnet holder 72 is rotated along the inner peripheral surface of the large-diameter portion 66 via the small gear 84 and the intermediate gear 80, and the polarity relationship of the outer ring magnet 76 with respect to the inner ring magnet 74. (N−N, N−S) changes. As a result, the strength of the magnetic field in the high magnetic flux density range α formed by the inner ring magnet 74 and the outer ring magnet 76 disposed with the conductor 50 interposed therebetween is reduced from, for example, a zero braking state where no braking force is formed. Further, it is possible to continuously change to the state of full braking that forms the maximum braking force.

  The braking force adjusting knob 82 is disposed so as to penetrate the support plate 60, is prevented from being removed by the retainer 86, and is energized between the plurality of recesses 82 a formed in the knob 82 and the support plate 60. Moderation is imparted in the rotational direction by the member 88 (comprising an engaging pin 88a and a spring 88b). The magnitude of the braking force generated by the rotation of the adjustment knob 82 can be set, for example, on a scale (not shown) every 10 steps or 20 steps according to the rotation position of the adjustment knob 82. That is, when this adjustment knob 82 is arranged at each scale position, a click moderation feeling can be obtained at each scale position.

Next, the operation of the dual bearing type reel 10 having the above-described configuration will be described.
When the spool shaft 14 and the spool 18 are stopped, as shown in FIG. 3A, the distal end (tip) of the second region 54 of the conductor 50 is in the high magnetic flux density range of the gap between the magnets 74 and 76. (Area between magnets 74 and 76) α does not enter and is outside. That is, the entire conductor 50 is outside the high magnetic flux density range α.

  For example, when the spool 18 is rotated by casting, the conductor 50 also rotates integrally with the spool 18. Since the centrifugal force acting on the centrifugal collar 44 is weak until the rotational speed of the spool 18 reaches a predetermined magnitude immediately after the start of casting, the pressing force of the centrifugal collar 44 against the tapered surface 18a of the spool 18 is weak. Is smaller than the biasing force of the spring member 48. Therefore, as shown in FIG. 3A, the conductor 50 hardly moves in the axial direction with respect to the spool shaft 14, and the conductor 50 has an annular shape formed between the inner magnet 74 and the outer magnet 76. It does not enter the high magnetic flux density range α which is a space.

  Thereafter, when the rotational speed of the spool 18 increases and the centrifugal force acting on the centrifugal collar 44 exceeds a predetermined magnitude, that is, the axial component of the pressing force of the centrifugal collar 44 against the tapered surface 18a of the spool 18 is a spring. When it becomes larger than the urging force of the member 48, the conductor 50 starts to move relative to the spool shaft 14 against the urging force of the spring member 48 due to the engagement guide action of the centrifugal collar 44 and the tapered surface 18a. That is, as the centrifugal force applied to the centrifugal collar 44 increases as the spool 18 rotates, the conductor 50 gradually moves to the left side in FIG. When the conductor 50 enters the high magnetic flux density range α (in the magnetic field by the magnets 74 and 76) by this movement, the amount of penetration (movement amount) and the rotation speed into the range α are entered into the conductor 50. The force corresponding to the is received from the magnetic field. Therefore, the braking force accompanying this force also acts on the spool 18 that rotates integrally with the conductor 50. That is, the magnetic braking force corresponding to the rotational speed of the spool 18 can be increased or decreased. As a result, the spool 18 is prevented from over-rotating and the backlash phenomenon is suppressed.

In this embodiment, the conductive member in the second region 54 has a lower specific gravity than the conductive member in the first region 52. For this reason, the moment of inertia of the second region 54 can be made smaller than the moment of inertia of the first region 52. Non-magnetic and low-conductivity materials have a wider selection range than non-magnetic and high-conductivity materials. For this reason, by using a material having a low specific gravity for the second region 54, the moment of inertia of the conductor 50 can be reduced, and the response of the rotational speed of the spool 18 to the braking force can be improved. . Further, by using a material having a small specific gravity for the conductive member in the second region 54, the weight of the conductor 50 as a whole can be reduced.
In addition, it is possible to suppress the tendency that the center of gravity position as the spool unit (the unit such as the spool 18, the conductor 50, and the spool shaft 14) is on the left side plate 10a side, and the load on both bearings 16a and 16b that support the spool unit. Balance is improved.
Further, the conductive member in the first region 52 has a Young's modulus greater than that of the conductive member in the second region 54. For this reason, the Young's modulus on the side where the bending moment is larger in the spool shaft 14 direction in the entire conductor 50 is large. Therefore, deformation of the conductor 50 can be suppressed, and the degree of freedom in design can be increased, for example, the distance between the conductor 50 and the magnets 74 and 76 can be reduced.

In the state shown in FIG. 3B, only the entire second region 54 of the conductor 50 is in the high magnetic flux density range α. Therefore, a braking force can be generated against the rotation of the conductor 50, that is, the rotation of the spool 18, but the second region 54 has a lower conductivity than the first region 52. The braking force when only the second region 54 is disposed in the high magnetic flux density range α is a state in which not only the second region 54 but also the first region 52 is disposed in the high magnetic flux density range α (FIG. 3 ( It is weaker than C).
When the rotation of the spool 18 is further increased, as shown in FIG. 3 (C), not only the second region 54 of the conductor 50 against the biasing force of the spring member 48 but also a higher conductivity than that. The first region 52 having the above is disposed in the high magnetic flux density range α. At this time, the first region 52 is more strongly affected by the magnets 74 and 76 than the second region 54. Therefore, the braking force against the rotation of the conductor 50, that is, the rotation of the spool 18, can be made larger than the state in which only the second region 54 is arranged in the high magnetic flux density range α. In particular, the conductor 50 moves to the left with respect to the magnets 74 and 76 after the boundary portion between the second region 54 and the first region 52 of the conductor 50 is disposed at the right end between the magnets 74 and 76. As you do, the braking force increases greatly. That is, the braking force between the state in which only the second region 54 is disposed between the magnets 74 and 76 and the state in which both the first and second regions 52 and 54 are disposed between the magnets 74 and 76 is used. A big difference can be given. When the state shown in FIG. 3C is maintained while the spool 18 rotates, the constant state is maintained with the braking force most increased.

  At the end of casting, the rotational speed of the spool 18 decreases and the centrifugal force acting on the centrifugal collar 44 becomes weak. Therefore, the axial component of the pressing force of the centrifugal collar 44 against the tapered surface 18a of the spool 18 is smaller than the biasing force of the spring member 48, and the conductor 50 is moved to the initial position by the biasing force of the spring member 48 (FIG. A) begin to be returned to see). As a result, the conductor 50 gradually gets out of the high magnetic flux density range α, and the force received from the magnetic field gradually decreases. In other words, the first region 52 having a high conductivity and receiving a large braking force by the magnets 74 and 76 comes out first from the high magnetic flux density range α. At this time, since the first region 52 comes out of the high magnetic flux density range α, the braking force suddenly decreases during that time, but the second region 54 maintains the state of being in the high magnetic flux density range α. A state where a braking force is applied to the conductor 50 can be maintained. Thus, the braking force on the conductor 50 is not changed suddenly from the strong state where the first region 52 is disposed in the high magnetic flux density range α to the state where the braking force is not applied at all. Since the region 54 is disposed in the high magnetic flux density range α, it is possible to prevent an abrupt and significant change in braking force in the low rotation speed region. Therefore, by providing the first and second regions 52 and 54 having different conductivities in the conductor 50, the braking force can be changed in two stages with respect to the spool 18, so that the flying distance can be reduced at the end of casting. Without reducing it unnecessarily, an appropriate braking force can be applied to the spool 18 to effectively prevent backlash.

As described above, the first region 52 and the second region 54 of the conductor 50 have different conductivities, so that each region 52 and 54 is different from the spool 18 every time it is disposed between the magnets 74 and 76. The braking performance can be exhibited.
Further, in the present embodiment, by rotating the braking force adjusting knob 82, the outer magnet 76 is rotated with respect to the inner magnet 74, whereby the polarity relationship (N−N, NS) can be changed. For this reason, the magnitude of the magnetic field formed between the inner magnet 74 and the outer magnet 76 can be adjusted, and a wide range of braking characteristics can be changed and set.

Next, a second embodiment will be described with reference to FIGS. 4A to 4C. This embodiment is a modification of the first embodiment.
When the spool 18 is in the stopped state, the second region 54 of the conductor 50 is within the high magnetic flux density range α that is affected by the magnets 74 and 76 as shown in FIG. As shown in FIG. 4B, the axial length of the second region 54 is substantially the same as the width L of the magnets 74 and 76. When the spring member 48 is most contracted, the distal end portion of the conductor 50 with respect to the centrifugal collar 44 is on the left side (left side plate 10a side) with respect to the left end portions of the magnets 74 and 76, as shown in FIG. Exit.

  As shown in FIG. 4A, the second region 54 of the conductor 50 is always within the high magnetic flux density range α between the magnets 74 and 76. For this reason, even in the initial stage immediately after the start of casting, the magnetic braking force corresponding to the rotational speed of the spool 18 can be increased or decreased. As a result, the spool 18 is prevented from over-rotating and the backlash phenomenon is suppressed. .

  As the rotational speed of the spool 18 increases and the centrifugal force acting on the centrifugal collar 44 exceeds a predetermined magnitude, and the centrifugal force applied to the centrifugal collar 44 as the spool 18 rotates, the conductor 50 increases. Gradually moves to the left in FIG. By this movement, the entire second region 54 of the conductor 50 enters the high magnetic flux density range α (inside the magnetic field by the magnets 74 and 76). For this reason, the conductor 50 receives a force corresponding to the amount of penetration (movement amount) and the rotational speed from the magnetic field. In this case, the conductivity from the distal end of the second region 54 to the boundary portion with the first region 52 is constant, but the amount of penetration of the second region 54 into the high magnetic flux density range α is different. A braking force that is gradually larger than the initial state (the state shown in FIG. 4A) is applied.

  Further, as the rotational speed of the spool 18 increases and the centrifugal force acting on the centrifugal collar 44 exceeds a predetermined magnitude, and the centrifugal force applied to the centrifugal collar 44 increases as the spool 18 rotates, the conductor 50 Gradually move to the left side in FIG. By this movement, not only the second region 54 of the conductor 50 but also the first region 52 enters the high magnetic flux density range α (in the magnetic field by the magnets 74 and 76). When the boundary portion between the second region 54 and the first region 52 enters the high magnetic flux density range α, the braking force rapidly increases. However, in the conductor 50, the second region 54 penetrates the left ends of the magnets 74 and 76 and moves to the left (back side). For this reason, although the amount of braking force of the penetrated portion is reduced, the braking force can be continuously increased even if the distal end of the conductor 50 exceeds the left end of the magnets 74 and 76.

  On the other hand, in the final stage of casting, the state in which the second region 54 is disposed between the magnets 74 and 76 can be maintained. Therefore, the rotation of the spool 18 with respect to the spool 18 from the beginning to the end of the casting is performed. The braking force according to the speed can be continuously applied.

Next, a third embodiment will be described with reference to FIGS. 5 (A) to 5 (C). This embodiment is a modification of the first and second embodiments.
As shown in FIGS. 5A to 5C, the conductor 50 includes a first region 52 near the support member 42a of the moving body 42, and a first region 52 on the distal end side (distal side) of the first region 52. In addition to the two regions 54, a third region 56 on the tip side (distal side) of the second region 54 is provided. In this embodiment, the thickness of the first region 52, the second region 54, and the third region 56 is the same, and between the first region 52 and the second region 54, the second region 54, The inner peripheral surface and the outer peripheral surface between the third region 56 are flush with each other. Further, the first region 52 and the second region 54 and the second region 54 and the third region 56 are fixed by appropriate means such as adhesion or fitting.
For example, a Cu alloy (JIS C1220T, conductivity 86 (IACS), specific gravity 8.94, Young's modulus 11800 (kgf / mm ² )) is used in the first region 52, and an Al alloy (JIS) is used in the second region 54. A2011-T3, conductivity 39 (IACS), specific gravity 2.82, Young's modulus 7200 (kgf / mm ² )), the third region 56 is, for example, Mg alloy (JIS AZ31, conductivity 17 (IACS), specific gravity 1 .78, Young's modulus 4500 (kgf / mm ² )) is used. That is, the first region 52 has the highest conductivity, and the conductivity decreases in the order of the second region 54 and the third region 56. Further, since the specific gravity is highest in the first region 52 and lower in the order of the second region 54 and the third region 56, the weight of the inertia can be reduced by reducing the weight of the conductor 50, and the braking can be reduced. Responsiveness can be improved. Further, since the position of the center of gravity as the spool unit can be brought closer to the center side of the spool shaft 14, the balance is improved, and the load balance to the bearings 16a and 16b supporting the spool unit is improved.

For example, in the initial state (see FIG. 5A), only the third region 56 enters the magnetic flux density range α (in the magnetic field by the magnets 74 and 76). Since the third region 56 has a low electrical conductivity, the braking action due to the rotation of the spool 18 is small.
As the spool 18 rotates, in addition to the third region 56, the second region 54 enters the magnetic flux density range α (inside the magnetic field by the magnets 74 and 76) as shown in FIG. Here, since the conductivity of the second region 54 is higher than that of the third region 56, the braking force is strengthened compared to the state shown in FIG.
When the rotation speed of the spool 18 further increases, as shown in FIG. 5C, the third region 56 protrudes to the left from the high magnetic flux density range α, and the entire second region 54 and a part of the first region 52 are formed. It is arranged within the magnetic flux density range α (in the magnetic field by the magnets 74 and 76). Here, since the conductivity of the second region 54 is higher than that of the third region 56 and the conductivity of the first region 52 is higher than that of the second region 54, the braking force is shown in FIG. It is strengthened from the state shown in.

As described above, by providing the first to third regions 52, 54, and 56 having different conductivities on the conductor 50, the braking force can be changed in three stages. Without reducing it unnecessarily, an appropriate braking force can be applied to the spool 18 to effectively prevent backlash.
In addition, since a part of the conductor 50 in this embodiment is always in the high magnetic flux density range α, a braking force can be applied from the beginning to the end of casting.

  Also in this embodiment, the Young's modulus of each of the regions 52, 54, and 56 is higher as the material on the spool 18 side. Therefore, since the Young's modulus on the side with the larger bending moment in the direction of the spool shaft 14 in the entire conductor 50 is large, the deformation of the conductor 50 can be suppressed, and the distance between the conductor 50 and the magnets 74 and 76. It is possible to increase the degree of freedom in design, such as making it possible to reduce.

Next, a fourth embodiment will be described with reference to FIGS. This embodiment is a modification of the first to third embodiments.
As shown in FIGS. 6 to 8, the support plate 60 of the magnetic braking device 40 of this embodiment is formed with a small-diameter portion 64 so as to surround the left end portion of the spool shaft 14. On the outer periphery of the small-diameter portion 64, a magnet holder (axial movement holding mechanism) 110 is provided that is fixed to the small-diameter portion 64 so as to be movable in the axial direction. In this case, the magnet holder 110 includes an inner annular wall 112 and an outer annular wall 114, and the inner annular wall 112 is fitted to the small diameter portion 64 so as to be movable in the axial direction. An inner magnet 74 is attached to the outer periphery of the inner annular wall 112 with a holder 116 interposed, and an outer magnet 76 is rotatably disposed on the inner periphery of the outer annular wall 114 with a holder 118 interposed. Has been.

  As shown in FIGS. 7 and 8, the inner annular wall 112 is formed with an annular recess (notch) 112 a that opens toward the spool 18, and a retainer 64 a attached to the tip of the small diameter portion 64. The magnet holder 110 is urged in the opposite direction to the spool 18 with an urging spring 112b interposed therebetween. The inner annular wall 112 is formed with a spiral cam surface 120 that opens toward the opposite side of the spool 18 and is annular and has a height difference along the circumferential direction.

  A knob 130 is rotatably mounted on the support plate 60 so as to enter the opening edge 11 of the left side plate 10a mounted on the support plate 60 so as to be exposed to the outside. The knob 130 is prevented from coming off when the flange 130 a faces the opening edge 11. Further, the knob 130 is integrally formed with an engaging projection 132 that engages with the helical cam surface 120 having the above-described height difference (see FIG. 9). The engagement relationship is always maintained with 132 by the biasing force of the biasing spring 112b.

  The adjusting knob 130 is imparted with moderation in the rotational direction by a biasing member 134 (comprising an engaging pin 134a and a spring 134b) interposed between the plurality of recesses 130b formed in the knob 130 and the support plate 60. ing. The magnitude of the braking force due to the rotation of the adjustment knob 130 can be set according to the rotational position of the adjustment knob 130. That is, when the adjusting knob 82 is arranged at each rotational position, a click moderation feeling can be obtained.

  By rotating the knob 130 with the above-described configuration, as shown schematically in FIG. 9, the magnet surface acts against the urging force of the urging spring 112b by the action of the cam surface 120 and the engagement protrusion 132, as shown in FIG. The holder 110 can be moved along the axial direction of the spool shaft 14 toward the spool 18 (in the direction of the arrow in FIG. 9). Further, by rotating the knob 130 in the reverse direction, the magnet holder 110 is spooled along the axial direction of the spool shaft 14 by the action of the cam surface 120 and the engaging projection 132 and the biasing force of the biasing spring 112b. 18 can be moved to the opposite side. In this case, by moving the magnet holding body 110 along the axial direction, the initial setting positions of the inner magnet 74 and the outer magnet 76 attached thereto with respect to the conductor 50 can be changed. It is possible to adjust the initial magnetic braking force and the final magnetic braking force acting on the body 50. FIG. 8 shows a state where the magnet holder 110 shown in FIG. 7 is moved to the spool 18 side along the axial direction.

  Further, in the present embodiment, as shown in FIG. 10, of the magnets 74 and 76 held by the magnet holder 110 described above, the outer magnet 76 (holder 118) is configured to be rotatable by the braking force adjusting knob 82. ing. Specifically, the intermediate gear 80 is attached to the outer peripheral surface of the holder 118 to which the outer magnet 76 is attached (may be integrally formed on the outer periphery of the holder 118), and the outer annular wall 114 of the magnet holder 110 is attached to the outer annular wall 114. An opening 114a extending in the axial direction is formed, and the intermediate gear 80 rotatably supported by the support plate 60 is meshed with the opening 114a.

  Further, by rotating the braking force adjusting knob 82 according to the configuration described in the first embodiment, as shown schematically in FIG. The holder 118 is rotated, that is, the outer magnet 76 is rotatable. In this case, by rotating the outer magnet 76, the polarity relationship (NN, NS) changes with the inner magnet 74, so that the magnetic braking force acting on the conductor 50 positioned between them is changed. It becomes possible to adjust.

As shown in FIG. 11A, the conductor 50 is formed such that the thickness t ₁ of the conductive member in the first region 52 is thicker than the thickness t ₂ of the conductive member in the second region 54. ing. In this embodiment, the inner peripheral surface of the first region 52 and the inner peripheral surface of the second region 54 are formed flush with each other. That is, the second region 54 is formed to be thin and the distance from the outer magnet 76 is increased. For this reason, the braking force when the second region 54 is disposed within the high magnetic flux density range α is weakened. On the other hand, the second region 52 is formed thick, and the distance from the outer magnet 76 is shorter than the second region 54. Therefore, the braking force when the first region 52 is disposed within the high magnetic flux density range α is increased. Moreover, weight reduction can be achieved by making the 2nd area | region 54 thin.

  For example, in the state shown in FIGS. 7 and 11A, when the spool 18 is rotated by casting, the moving body 42 is also integrally rotated with the spool 18. After that, when the rotational speed of the spool 18 increases and the centrifugal force acting on the centrifugal collar 44 exceeds a predetermined magnitude, the second region 54 of the conductor 50 becomes the inner magnet 74 as shown in FIG. And in the high magnetic flux density range α formed between the outer magnets 76. At this time, since the conductive member in the second region 54 has a low conductivity and is formed thin, a small braking force can be applied.

When the spool 18 is further rotated at a high speed, the entire second region 54 of the conductor 50 is disposed within a high magnetic flux density range α formed between the inner magnet 74 and the outer magnet 76 as shown in FIG. The At this time, only the second region 54 is disposed within the high magnetic flux density range α between the magnets 74 and 76, and the first region 52 is not disposed, so that the braking force applied to the conductor 50 is the spool. It can be applied in any of the 18 rotation regions. Note that the braking force gradually increases according to the amount of the second region 54 disposed between the magnets 74 and 76.
Therefore, when used in the state shown in FIGS. 7 and 11, it is suitable for casting a lure having a relatively light weight or casting in a tailwind.

Then, the magnetic braking device 40 operates the knob 130 to move the positions of the magnets 74 and 76 from the position shown in FIG. 7 to the position shown in FIG.
At this time, since a part of the second region 54 is disposed in the high magnetic flux density range α, a weak braking force is applied to the conductor 50 from the initial casting state (see FIG. 12A). .

  Thereafter, when the rotational speed of the spool 18 increases and the centrifugal force acting on the centrifugal collar 44 exceeds a predetermined magnitude, the entire second region 54 of the conductor 50 becomes the inner magnet as shown in FIG. 74 and the outer magnet 76 are disposed in a high magnetic flux density range α. At this time, since the conductive member in the second region 54 is formed thin, a small braking force can be applied.

When the spool 18 is further rotated at a high speed, as shown in FIG. 12C, not only the second region 54 of the conductor 50 but also the first region 52 is formed with a high magnetic flux formed between the inner magnet 74 and the outer magnet 76. It arrange | positions in the density range (alpha). At this time, the first region 52 has high conductivity and is formed thick, so that the braking force when placed in the high magnetic flux density range α is strengthened. Therefore, when the first region 52 is disposed within the high magnetic flux density range α, the braking force increases rapidly.
Therefore, when used in the state shown in FIG. 8 and FIG. 12, it is suitable for casting a lure having a relatively heavy weight or casting in a headwind.

According to this embodiment, by rotating the knob 130 to move the magnet holder 110, the magnets 74 and 76 are brought close to the spool 18 from the state shown in FIG. 7 to the state shown in FIG. The magnets 74 and 76 can be separated from the spool 18 from the state shown in FIG. At this time, since it becomes possible to change and set the braking characteristics from the initial stage to the middle period and from the middle period to the final stage of the rotation of the spool 18, it is possible to respond widely from short cast to long cast according to various changes in the fishing grounds. It becomes possible. As described above, the initial setting positions of the inner magnet 74 and the outer magnet 76 can be changed by the magnet holder 110, so that the braking characteristics can be adjusted according to various casting conditions (such as charging method, used lure, and wind direction). The optimal state can be set.
Further, by operating the knob 82 described in the first embodiment together, it is possible to deal more precisely from short cast to long cast.

Next, a fifth embodiment will be described with reference to FIG. This embodiment is a modification of the first to fourth embodiments.
As shown in FIG. 13, the conductor 50 of this embodiment includes a first conductive member 92 and a second conductive member 94. As the first conductive member 92, one having higher conductivity than the second conductive member 94 is used. For example, a Cu alloy (JIS C1220T, conductivity 86 (IACS), specific gravity 8.94, Young's modulus 11800 (kgf / mm ² )) is used for the first conductive member 92, and the second conductive member 94 is used. Al alloy (JIS A2011-T3, electrical conductivity 39 (IACS), specific gravity 2.82, Young's modulus 7200 (kgf / mm ² )) is used for.

The first conductive member 92 has a cylindrical shape, is supported by the support member 42 a of the moving body 42, and extends between the magnets 74 and 76 from the side close to the spool 18. An annular recess 92 a is formed on the outer peripheral surface of the first conductive member 92. The second conductive member 94 is formed in a cylindrical shape, and is disposed in the recess 92 a on the outer peripheral surface of the first conductive member 92. The second conductive member 94 is fixed to the concave portion 92a of the first conductive member 92, for example, by adhesion.
In this embodiment, the outer peripheral surface of the first conductive member 92 other than the recess 92a and the outer peripheral surface of the second conductive member 94 are flush with each other. Further, the distal end portion of the first conductive member 92 with respect to the spool 18 and the distal end portion of the second conductive member 94 with respect to the spool 18 are substantially flush with each other.

A region from the portion of the first conductive member 92 supported by the support member 42 a of the moving body 42 to the proximal end portion of the second conductive member 94 is defined as the first region 52. A range in which the first conductive member 92 and the second conductive member 94 are overlapped is defined as a second region 54.
That is, the electric conductor 50 according to this embodiment has cylindrical first and second regions 52 and 54, respectively. Here, since the first region 52 is formed of a single material, the conductivity is constant. In the second region 54, the conductivity of the same material (first conductive member 92) as the first region 52 is σ ₁ and the thickness is t ₁ . In the second region 54, the conductivity of the second conductive member 94 is σ ₂ and the thickness is t ₂ . Then, the electrical conductivity σ of the second region 54 can be obtained as follows.
σ = (t ₁ σ ₁ + t ₂ σ ₂ ) / (t ₁ + t ₂ )
Note that the conductivity σ of the second region 54 is constant within the range of the second region 54. Since the conductivity of the second conductive member 94 is lower than the conductivity of the first conductive member 92, the conductivity σ of the second region 54 is smaller than the conductivity of the first region 52. .
Since the operation of this embodiment is the same as that described in the first embodiment, a detailed description thereof will be omitted.

Thus, by forming the first and second conductive members 92 and 94, the conductor 50 can be easily manufactured with high accuracy.
Note that the second conductive member 94 disposed in the recess 92a on the outer peripheral surface of the first conductive member 92 may be detachable by fitting or the like. Then, the second conductive member 94 can be appropriately selected and the conductivity of the second region 54 can be appropriately set.

Next, a sixth embodiment will be described with reference to FIG. This embodiment is a modification of the fifth embodiment.
For example, a Cu alloy (JIS C1220T, conductivity 86 (IACS), specific gravity 8.94, Young's modulus 11800 (kgf / mm ² )) is used for the first conductive member 92 shown in FIG. An Al alloy (JIS A2011-T3, conductivity 39 (IACS), specific gravity 2.82, Young's modulus 7200 (kgf / mm ² )) is used for the conductive member 94.
In this embodiment, the position of the distal end of the first conductive member 92 relative to the spool 18 is positioned away from the spool 18 relative to the distal end of the second conductive member 94 relative to the spool 18 ( Distal).

A region from the portion of the first conductive member 92 supported by the support member 42 a of the moving body 42 to the proximal end portion of the second conductive member 94 is defined as the first region 52. A range in which the first conductive member 92 and the second conductive member 94 are overlapped is defined as a second region 54. A region from the distal end portion of the second conductive member 94 to the distal end portion of the first conductive member 92 in the first conductive member 92 is defined as a third region 56.
That is, the conductor 50 according to this embodiment has first to third regions 52, 54, and 56 that are cylindrical. Here, since the first region 52 and the third region 56 are formed of a single material, the conductivity is constant. The conductivity σ of the second region 54 can be obtained as described in the fifth embodiment, and is constant within the range of the second region 54.

  Here, the first region 52 and the third region 56 have the same conductivity because the first conductive member 92 is used, but the first region 52 is thicker than the third region 56. It is. For this reason, the distance between the inner magnet 74 and the first and third regions 52 and 56 of the conductor 50 is the same, but the distance between the outer magnet 76 and the third region 56 of the conductor 50 is The distance is larger than the distance between the outer magnet 76 and the first region 52 of the conductor 50. That is, the third region 56 of the conductor 50 is farther than the first region 52 in relation to the outer magnet 76.

  As described above, when the distance between the outer magnet 76 and the third region 56 of the conductor 50 is larger than the distance between the outer magnet 76 and the first region 52 of the conductor 50, the conductor 50 is changed. The magnetic flux density that passes is reduced. Therefore, the magnetic force acting on the conductor 50, that is, the magnetic braking force acting on the spool 18 is also smaller in the third region 56 than in the first region 52. Therefore, if the thickness of the first region 52 and the third region 56 is the same, the conductivity of the third region 56 is the same as that of the first region 52 is lower.

  In this embodiment, the case where the second conductive member 94 is used in the second region 54 has been described. However, another conductive member (not shown) (not shown in the second conductive member 94) is used in the third region 56. Also, for example, conductivity may be low).

By using the conductor 50 having a plurality of regions in the direction along the axial direction of the spool shaft 14 as described above, various brake characteristics can be set and various casting scenes can be handled. it can. In the fishing reel 10 according to the first to sixth embodiments, the spool 18 can be replaced, and the spool 18 having various conductors 50 can be used. Then, it can respond flexibly to more various casting scenes.
Although several embodiments have been specifically described so far with reference to the drawings, the present invention is not limited to the above-described embodiments, and all the embodiments performed without departing from the scope of the invention are described. Including implementation.

  DESCRIPTION OF SYMBOLS 10 ... Fishing reel, 10a, 10b ... Side plate, 12 ... Reel body, 12a, 12b ... Frame, 14 ... Spool shaft, 16a, 16b ... Bearing, 18 ... Spool, 18a ... Tapered surface, 40 ... Magnetic brake device, 42 ... moving body, 42a ... support member, 44 ... centrifugal collar, 44a ... inclined surface, 46 ... retainer, 48 ... spring member, 50 ... conductor, 52 ... first region, 54 ... second region, 60 ... support plate , 60a ... opening, 62 ... central opening, 64 ... small diameter part, 66 ... large diameter part, 68 ... support base part, 70 ... annular groove, 72 ... magnet holder, 74 ... inner ring magnet, 76 ... outer ring magnet, 78 ... tooth, 80 ... intermediate gear, 82 ... braking force adjusting knob, 84 ... small gear.

Claims (6)

A non-magnetic conductor, which is prevented from rotating on the spool shaft, can move in a direction away from the spool along the axial direction of the spool shaft by centrifugal force accompanying the rotation of the spool, and the conductor is between the opposing magnets. In a fishing reel having a magnetic braking device that magnetically brakes rotation of the spool via the conductor when in a magnetic field,
The conductor has at least two regions each having a different conductivity;
The fishing reel according to claim 1, wherein the at least two regions can be disposed in a magnetic field between the magnets.   2. The fishing reel according to claim 1, wherein the conductor has a conductivity in a region close to the spool higher than a conductivity in a region separated from the spool.   3. The fishing reel according to claim 1, wherein the conductor has a specific gravity of a region close to the spool higher than a specific gravity of a region separated from the spool. 4. The conductor is cylindrical, and is disposed on the outer side of the first conductive member disposed from the side close to the spool to the side separated from the spool, and the side of the first conductive member separated from the spool. A second conductive member provided,
The conductor is
A first region defined in a range of an end portion of the first conductive member close to the spool from a side close to the spool, of the second conductive member;
The first and second conductive members form a second region defined within the overlapped range, and the conductivity is constant in each region. The fishing reel according to claim 3. The opposing magnets each have a width in the direction of movement of the conductor,
When the conductor moves in a direction away from the spool, the side of the conductor that is separated from the spool can penetrate through the magnetic field of the opposing magnet and move deeper than the width of the magnet. The fishing reel according to any one of claims 1 to 4, wherein:   6. The magnetic braking device according to claim 1, further comprising an axial movement holding mechanism that holds the opposing magnets so as to be movable in the axial direction of the spool shaft. 7. Fishing reel.

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